We report on the creation and characterization of heteronuclear
40K87Rb Feshbach molecules in an optical dipole trap. Starting from an ultracold gas mixture of
40K and
87Rb atoms, we create as many as 25 000 molecules at 300 nK by rf association. Optimizing the association process, we achieve a conversion efficiency of 25%. We measure the temperature dependence of the rf association process and find good agreement with a phenomenological model that has previously been applied to Feshbach molecule creation by slow magnetic-field sweeps. We also present a measurement of the binding energy of the heteronuclear molecules in the vicinity of the Feshbach resonance and provide evidence for Feshbach molecules as deeply bound as 26 MHz.
We report on the creation of ultracold gases of bosonic Feshbach molecules of NaCs.The molecules are associated from overlapping gases of Na and Cs using a Feshbach resonance at 864.12(5) G.We characterize the Feshbach resonance using bound-state spectroscopy, in conjunction with a coupled-channel calculation.By varying the temperature and atom numbers of the initial atomic mixtures, we demonstrate the association of NaCs gases over a wide dynamic range of molecule numbers and temperatures, reaching 70 nK for our coldest systems and a phase-space density near 0.1.This is an important stepping stone for the creation of degenerate gases of strongly dipolar NaCs molecules in their absolute ground state.
We report on the observation of ultracold heteronuclear Feshbach molecules. Starting with a
87Rb Bose-Einstein condensate and a cold atomic gas of
85Rb, we utilize previously unobserved interspecies Feshbach resonances to create up to 25 000 molecules. Even though the
85Rb gas is nondegenerate, we observe a large molecular conversion efficiency due to the presence of a quantum degenerate
87Rb gas; this represents a key feature of our system. We compare the molecule creation at two different Feshbach resonances with different magnetic-field widths. The two Feshbach resonances are located at $265.44\ifmmode\pm\else\textpm\fi{}0.15\text{ }\mathrm{G}$ and $372.4\ifmmode\pm\else\textpm\fi{}1.3\text{ }\text{ }\mathrm{G}$. We also directly measure the small binding energy of the molecules through resonant magnetic-field association.